scholarly journals From chaotic spin dynamics to noncollinear spin textures in YIG nanofilms by spin-current injection

2020 ◽  
Vol 102 (17) ◽  
Author(s):  
Henning Ulrichs
2021 ◽  
Author(s):  
◽  
Geert Hoogeboom

Ferromagnets (FMs) have been a key ingredient in information technology because it is easy to manipulate and read out the magnetization. Antiferromagnets (AFMs) have magnetic moments with alternating direction resulting in negligible magnetization. This gives them high processing and device downscaling features, but this also makes it challenging to manipulate and interact with the AFM order. This thesis studies this interaction with antiferromagnets. NiO AFM order has been read out by electrically injecting spin current via the spin Hall effect in thin heavy metal films. In DyFeO3, both Dy and Fe magnetic moments, their excitation and interaction have been probed. A magnetic field lifts the degeneracy of magnetic excitations with opposite magnon spin, allowing a spin current to be detected nonlocally. The AFM order and the generation of spin current can easily be controlled by an adjacent FM. Thereby, we show that AFMs have the potential to play an active role in spintronics.


AIP Advances ◽  
2016 ◽  
Vol 7 (5) ◽  
pp. 055808 ◽  
Author(s):  
S. Oki ◽  
T. Kurokawa ◽  
S. Honda ◽  
S. Yamada ◽  
T. Kanashima ◽  
...  

AIP Advances ◽  
2018 ◽  
Vol 8 (1) ◽  
pp. 015131 ◽  
Author(s):  
Haiqing Xie ◽  
Fuming Xu ◽  
Hujun Jiao ◽  
Qiang Wang ◽  
J.-Q. Liang

2012 ◽  
Vol 111 (7) ◽  
pp. 07C513 ◽  
Author(s):  
G. L. da Silva ◽  
L. H. Vilela-Leão ◽  
S. M. Rezende ◽  
A. Azevedo

2005 ◽  
Vol 86 (12) ◽  
pp. 122103 ◽  
Author(s):  
E. Ya. Sherman ◽  
Ali Najmaie ◽  
J. E. Sipe

Author(s):  
E. Saitoh ◽  
K. Ando

This chapter describes an experiment on the inverse spin Hall effect (ISHE) induced by spin pumping. Spin pumping is the generation of spin currents as a result of magnetization M(t) precession; in a ferromagnetic/paramagnetic bilayer system, a conduction-electron spin current is pumped out of the ferromagnetic layer into the paramagnetic conduction layer in a ferromagnetic resonance condition. The sample used in the experiment is a Ni81Fe19/Pt bilayer film comprising a 10-nm-thick ferromagnetic Ni81Fe19layer and a 10-nm-thick paramagnetic Pt layer. For the measurement, the sample system is placed near the centre of a TE011 microwave cavity at which the magnetic-field component of the microwave mode is maximized while the electric-field component is minimized.


2020 ◽  
Vol 124 (2) ◽  
Author(s):  
Angela Wittmann ◽  
Guillaume Schweicher ◽  
Katharina Broch ◽  
Jiri Novak ◽  
Vincent Lami ◽  
...  

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